2007/08/31 by M. M. Korshunov, Ilya Eremin, I. Eremin · 2 citations
Materials Science · Physics and Astronomy · #Advanced Condensed Matter Physics #Magnetic and transport properties of perovskites and related materials #Physics of Superconductivity and Magnetism #cond-mat.str-el #cond-mat.supr-con
paper · pdf · doi:10.1103/physrevb.77.064510
published as Phys. Rev. B 77, 064510 (2008) · Published version, PACS: 74.70.-b; 75.40.Gb; 74.20.Rp; 74.25.Jb
openalex publication_date 2008/02/15 · arxiv created 2008/02/18 · arxiv updated 2009/12/01 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/28
We systematically analyze the influence of the superconducting gap symmetry and the electronic structure on the dynamical spin susceptibility in superconducting NaxCoO2\ensuremath⋅yH2O within three different models: The single a1g-band model with nearest-neighbor hoppings, the realistic three-band t2g model with, and without eg^\ensuremath' pockets present at the Fermi surface. We show that the magnetic response in the normal state is dominated by the incommensurate antiferromagnetic spin density wave fluctuations at large momenta in agreement with experimental temperature dependence of the spin-lattice relaxation rate. Also, we demonstrate that the presence or the absence of the eg^\ensuremath' pockets at the Fermi surface does not significantly affect this conclusion. In the superconducting state our results for d_x2\ensuremath-y2- or dxy-wave symmetries of the superconducting order parameter are consistent with experimental data and exclude nodeless d_x2\ensuremath-y2+idxy-wave symmetry. We further point out that the spin-resonance peak proposed earlier is improbable for the realistic band structure of NaxCoO2\ensuremath⋅yH2O. Moreover, even if present the resonance peak is confined to the antiferromagnetic wave vector and disappears away from it.